Geometric phase transferred from photonic mode to atomic BEC

Standard

Geometric phase transferred from photonic mode to atomic BEC. / Yakovleva, T. S.; Rostom, A. M.; Tomilin, V. A. и др.

в: Optics Communications, Том 436, 01.04.2019, стр. 52-56.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Yakovleva, TS, Rostom, AM , Tomilin, VA & Il'ichov, LV 2019, 'Geometric phase transferred from photonic mode to atomic BEC', Optics Communications, Том. 436, стр. 52-56. https://doi.org/10.1016/j.optcom.2018.12.001

APA

Yakovleva, T. S., Rostom, A. M., Tomilin, V. A., & Il'ichov, L. V. (2019). Geometric phase transferred from photonic mode to atomic BEC. Optics Communications, 436, 52-56. https://doi.org/10.1016/j.optcom.2018.12.001

Vancouver

Yakovleva TS, Rostom AM , Tomilin VA , Il'ichov LV. Geometric phase transferred from photonic mode to atomic BEC. Optics Communications. 2019 апр. 1;436:52-56. doi: 10.1016/j.optcom.2018.12.001

Author

Yakovleva, T. S. ; Rostom, A. M. ; Tomilin, V. A. и др. / Geometric phase transferred from photonic mode to atomic BEC. в: Optics Communications. 2019 ; Том 436. стр. 52-56.

BibTeX

@article{3f4738c4f66e42a09b2a40039025b15e,

title = "Geometric phase transferred from photonic mode to atomic BEC",

abstract = "A process of geometric phase generation in a composite matter-field system is considered. Two atomic modes correspond to different localizations of a single Bose–Einstein condensate (BEC). One of the trapping localizations is formed by a photonic mode of a ring cavity. The photonic mode is governed by an external harmonic field source, by dissipation and by the number of localized atoms due to their non-resonant interaction with photons. This interaction gives rise to entanglement between the BEC and the photonic mode. By varying the intensity and frequency of the external source, it is possible to create a geometric phase for the optical mode. Because of the entanglement between the state of atomic and photonic modes, geometric phase acquired by the latter causes modification of the BEC state. This modification can be revealed by studying the tunneling between the atomic localizations.",

keywords = "Bose–Einstein condensate, Geometric phase, Two-mode approximation",

author = "Yakovleva, {T. S.} and Rostom, {A. M.} and Tomilin, {V. A.} and Il'ichov, {L. V.}",

note = "Publisher Copyright: {\textcopyright} 2018 Elsevier B.V.",

year = "2019",

month = apr,

day = "1",

doi = "10.1016/j.optcom.2018.12.001",

language = "English",

volume = "436",

pages = "52--56",

journal = "Optics Communications",

issn = "0030-4018",

publisher = "Elsevier",

}

RIS

TY - JOUR

T1 - Geometric phase transferred from photonic mode to atomic BEC

AU - Yakovleva, T. S.

AU - Rostom, A. M.

AU - Tomilin, V. A.

AU - Il'ichov, L. V.

PY - 2019/4/1

Y1 - 2019/4/1

N2 - A process of geometric phase generation in a composite matter-field system is considered. Two atomic modes correspond to different localizations of a single Bose–Einstein condensate (BEC). One of the trapping localizations is formed by a photonic mode of a ring cavity. The photonic mode is governed by an external harmonic field source, by dissipation and by the number of localized atoms due to their non-resonant interaction with photons. This interaction gives rise to entanglement between the BEC and the photonic mode. By varying the intensity and frequency of the external source, it is possible to create a geometric phase for the optical mode. Because of the entanglement between the state of atomic and photonic modes, geometric phase acquired by the latter causes modification of the BEC state. This modification can be revealed by studying the tunneling between the atomic localizations.

AB - A process of geometric phase generation in a composite matter-field system is considered. Two atomic modes correspond to different localizations of a single Bose–Einstein condensate (BEC). One of the trapping localizations is formed by a photonic mode of a ring cavity. The photonic mode is governed by an external harmonic field source, by dissipation and by the number of localized atoms due to their non-resonant interaction with photons. This interaction gives rise to entanglement between the BEC and the photonic mode. By varying the intensity and frequency of the external source, it is possible to create a geometric phase for the optical mode. Because of the entanglement between the state of atomic and photonic modes, geometric phase acquired by the latter causes modification of the BEC state. This modification can be revealed by studying the tunneling between the atomic localizations.

KW - Bose–Einstein condensate

KW - Geometric phase

KW - Two-mode approximation

UR - http://www.scopus.com/inward/record.url?scp=85058003152&partnerID=8YFLogxK

U2 - 10.1016/j.optcom.2018.12.001

DO - 10.1016/j.optcom.2018.12.001

M3 - Article

AN - SCOPUS:85058003152

VL - 436

SP - 52

EP - 56

JO - Optics Communications

JF - Optics Communications

SN - 0030-4018

ER -

ID: 18068574